Magnetic material for magnetic refrigeration

ABSTRACT

A magnetic material for magnetic refrigeration has a composition represented by (R1 1-y R2 y ) x Fe 100-x  (R1 is at least one of element selected from Sm and Er, R2 is at least one of element selected from Ce, Pr, Nd, Tb and Dy, and x and y are numerical values satisfying 4≦x≦20 atomic % and 0.05≦y≦0.95), and includes a Th 2 Zn 17  crystal phase, a Th 2 Ni 17  crystal phase, or a TbCu 7  crystal phase as a main phase.

CROSS-REFERENCE TO RELATED APPLICATIONS

This application is based upon and claims the benefit of priority fromthe prior Japanese Patent Application No. 2006-086421 filed on Mar. 27,2006; the entire contents of which are incorporated herein by reference.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The present invention relates to a magnetic material used for magneticrefrigeration.

2. Description of the Related Art

Most of refrigeration technologies for use in a room temperature regionsuch as refrigerators, freezers, and air-conditioners use a gascompression cycle. But, the refrigeration technologies based on the gascompression cycle have a problem of causing environmental destructionassociated with the exhaustion of specific freon gases to theenvironment, and there is also concern that substitute freon gases havean adverse effect upon the environment. Under the circumstancesdescribed above, clean and highly efficient refrigeration technologies,which are free from environmental problems caused by wastage ofoperating gases, have been demanded to be put into practical use.

Recently, magnetic refrigeration is being increasingly expected as oneof such environment-friendly, highly efficient refrigerationtechnologies. Research and development of magnetic refrigerationtechnologies for use in a room temperature region is underway. Themagnetic refrigeration technologies use the magnetocaloric effect ofmagnetic material instead of freon gases or substitute freon gases as arefrigerant to realize a refrigeration cycle. Specifically, therefrigeration cycle is realized by using a magnetic entropy change (ΔS)of the magnetic material associated with a magnetic phase transition(phase transition between a paramagnetic state and a ferromagneticstate). In order to realize the highly efficient magnetic refrigeration,it is preferable to use a magnetic material which exhibits a highmagnetocaloric effect around room temperature.

As such a magnetic material, a single rare earth element such as Gd, arare earth alloy such as Gd—Y alloy or Gd—Dy alloy, Gd₅ (Ge, Si)₄ basedmaterial, La (Fe, Si)₁₃ based material, Mn—As—Sb based material and thelike are known (JP-A 2002-356748 (KOKAI) and JP-A 2003-096547 (KOKAI)).The magnetic phase transition of the magnetic material is in two typesincluding a first order type and a second order type. The Gd₅ (Ge, Si)₄based material, the La(Fe, Si)₁₃ based material and the Mn—As—Sb basedmaterial exhibit the first order magnetic phase transition. Thesemagnetic materials can be used to easily obtain a large entropy change(ΔS) by the application of a low magnetic field but has a practicalproblem that its operating temperature range is narrow.

A rare earth metal such as Gd and a rare earth alloy such as Gd—Y alloyor Gd—Dy alloy exhibit the second order magnetic phase transition, sothat they have advantages that they can operate in a relatively widetemperature range and also have a relatively large entropy change (ΔS).But, the rare earth element itself is expensive, and when the rare earthelement or the rare earth alloy is used as a magnetic material formagnetic refrigeration, it is inevitable that the cost of the magneticmaterial for magnetic refrigeration becomes high.

Besides, it is also known that a (Ce_(1-x)Y_(x))₂Fe₁₇ (x=0 to 1) basedmagnetic material exhibits the second order magnetic phase transition.The (Ce, Y)₂Fe₁₇ based magnetic material can operate in a relativelywide temperature range in the same manner as the rare earth element andthe rare earth alloy, and it is a substance based on inexpensive Fe, sothat the cost of the magnetic material for magnetic refrigeration can bemade lower than the rare earth metal or the rare earth alloy. However,the (Ce, Y)₂Fe₁₇ based magnetic material has high magnetic anisotropy,so that it has a disadvantage that a magnetic entropy change amount (ΔS)associated with the magnetic phase transition is small.

SUMMARY OF THE INVENTION

A magnetic material for magnetic refrigeration according to an aspect ofthe present invention has a composition represented by a generalformula:

(R1_(1-y)R2_(y))_(x)Fe_(100-x)

(where, R1 is at least one of element selected from Sm and Er, R2 is atleast one of element selected from Ce, Pr, Nd, Tb and Dy, and x and yare numerical values satisfying 4≦x≦20 atomic % and 0.05≦y≦0.95), andincludes a Th₂Zn₁₇ crystal phase, a Th₂Ni₁₇ crystal phase or a TbCu₇crystal phase as a main phase.

A magnetic material for magnetic refrigeration according to anotheraspect of the present invention has a composition represented by ageneral formula:

(R1_(1-y)X_(y))_(x)Fe_(100-x)

(where, R is at least one of element selected from La, Ce, Pr, Nd, Sm,Gd, Tb, Dy, Ho, Er, Tm, Yb and Y, X is at least one of element selectedfrom Ti, Zr and Hf, and x and y are numerical values satisfying 4≦x≦20atomic % and 0.01≦y≦0.9), and includes a Th₂Ni₁₇ crystal phase or aTbCu₇ crystal phase as a main phase.

BRIEF DESCRIPTION OF THE DRAWING

FIG. 1 is a diagram showing Curie temperatures in R—Fe based materialsand 4f electron orbits of rare earth elements R.

DETAILED DESCRIPTION OF THE INVENTION

Hereinafter, embodiments of the present invention are described. Amagnetic material for magnetic refrigeration according to a firstembodiment has a composition expressed by the following general formula:

(R1_(1-y)R2_(y))_(x)Fe_(100-x)  (1)

(where, R1 is at least one of element selected from Sm and Er, R2 is atleast one of element selected from Ce, Pr, Nd, Tb and Dy, and x and yare numerical values satisfying 4≦x≦20 atomic % and 0.05≦y≦0.95), andincludes a Th₂Zn₁₇ crystal phase, a Th₂Ni₁₇ crystal phase or a TbCu₇crystal phase as a main phase.

The magnetic material for magnetic refrigeration is a material having arare earth element (element R) and iron (Fe) as main components andinexpensive Fe as a base. Specifically, the second order magnetic phasetransition is realized by a magnetic material having the rare earthelement in a small amount. In order to realize the second order magneticphase transition by such material, the magnetic material for magneticrefrigeration has a Th₂Zn₁₇ crystal phase (phase having a Th₂Zn₁₇ typecrystal structure), a Th₂Ni₁₇ crystal phase (phase having a Th₂Ni₁₇ typecrystal structure), or a TbCu₇ crystal phase (phase having a TbCu₇ typecrystal structure) as a main phase. The main phase shall be a phaseoccupying a maximum volume among the constituent phases (includingcrystal phases and amorphous phases) of the magnetic material formagnetic refrigeration.

The magnetic material having the Th₂Zn₁₇ crystal phase has the element Rmainly entered a position corresponding to the Th of the Th₂Zn₁₇ crystalphase, and the Fe mainly entered a position corresponding to the Zn ofthe Th₂Zn₁₇ crystal phase. Similarly, the magnetic material having theTh₂Ni₁₇ crystal phase has the element R mainly entered a positioncorresponding to the Th, and the Fe mainly entered a positioncorresponding to the Ni. The magnetic material having the TbCu₇ crystalphase has the element R mainly entered a position corresponding to theTb, and the Fe mainly entered a position corresponding to the Cu.

The magnetic material of the first embodiment has the rare earth elementin a small content as indicated by a site occupying atom of each crystalphase and an atom ratio between the element R and Fe based on it, sothat the second order magnetic phase transition is realized by aninexpensive material. To realize the magnetic material exhibiting thesecond order magnetic phase transition by using the Th₂Zn₁₇ crystalphase, the Th₂Ni₁₇ crystal phase or the TbCu₇ crystal phase as the mainphase, the value x in the formula (1) shall be in a range from 4 to 20atomic %. When the value x is less than 4 atomic % or exceeds 20 atomic%, the magnetic material having the Th₂Zn₁₇ crystal phase, the Th₂Ni₁₇crystal phase or the TbCu₇ crystal phase as the main phase cannot berealized. The value x is more preferably in a range from 8 to 15 atomic%.

The main phase of the magnetic material may be anyone of the Th₂Zn₁₇crystal phase, the Th₂Ni₁₇ crystal phase and the TbCu₇ crystal phase. Byusing anyone of these crystal phases as the main phase, the magneticmaterial exhibiting the second order magnetic phase transition can berealized. But, the TbCu₇ crystal phase is a high-temperature phase, anda rapid solidification step or the like is required to stabilize it in anormal temperature range. Meanwhile, the Th₂Zn₁₇ crystal phase and theTh₂Ni₁₇ crystal phase are stable under normal temperature. To reduce theproduction cost of the magnetic material, it is preferable that themagnetic material has the Th₂Zn₁₇ crystal phase or the Th₂Ni₁₇ crystalphase as the main phase.

It depends on the kind of rare earth element R as shown in FIG. 1whether the main phase of the magnetic material becomes the Th₂Zn₁₇crystal phase or the Th₂Ni₁₇ crystal phase. When the rare earth elementR is Ce, Pr, Nd, Sm or the like, it becomes the Th₂Zn₁₇ crystal phase.If the rare earth element R is Tb, Dy, Ho, Er or the like, it becomesthe Th₂Ni₁₇ crystal phase. As described later, the element R2 ispreferably at least one selected from Ce, Pr and Nd. Therefore, it ispreferable that the main phase of the magnetic material is the Th₂Zn₁₇crystal phase.

In a case where the magnetic material is used as a magneticrefrigeration material, a temperature (Curie temperature) indicating themagnetic phase transition (phase transition between a paramagnetic stateand a ferromagnetic state) and a magnitude (ΔS) of the magnetic entropychange associated with the magnetic phase transition are significant.FIG. 1 shows a Curie temperature of the R—Fe based material to whichvarious kinds of rare earth elements R are applied. As shown in FIG. 1,the application of Ce, Pr, Nd, Sm, Tb, Dy or Er as the element R cancontrol the Curie temperature of the magnetic material to be close toroom temperature. When the Curie temperature is close to roomtemperature, it means that the magnetocaloric effect can be obtainednear room temperature. The Curie temperature of the magnetic material ispreferably 320K or less, and more preferably 250K or more and 320K orless in view of improvement of its usefulness as the magneticrefrigeration material. The Curie temperature of the magnetic materialis more preferably 270K or more.

The magnetic entropy change amount (ΔS) associated with the magneticphase transition is affected by the magnetic anisotropy of the magneticmaterial. In other words, a large magnetic entropy change amount (ΔS)can be obtained by reducing the magnetic anisotropy of the magneticmaterial. Here, the individual figures (spherical, vertically long ovalor horizontally long oval) shown in FIG. 1 indicate 4f electron orbitsof the rare earth element R. For example, the 4f electron orbit of Gd iscircular, indicating that the magnetic anisotropy is small. Therefore,the R—Fe based material to which Gd is applied as the R element has alarge magnetic entropy change amount (ΔS). But, the Gd—Fe based materialis poor in usability because the Curie temperature is excessively high.

The 4f electron orbits of Sm and Er indicate cigar like long electronorbits, and those of Ce, Pr, Nd, Tb and Dy indicate pancake-likeflattened electron orbits. The R—Fe based material independently usingthese rare earth elements R has a large magnetic anisotropy and,therefore, a sufficient magnetic entropy change amount (ΔS) cannot beobtained. Meanwhile, where at least one of element R1 selected from Smand Er and at least one of element R2 selected from Ce, Pr, Nd, Tb andDy are used as a mixture, the 4f electron orbit is adjusted by a longelectron orbit and a flattened electron orbit, so that the magneticanisotropy can be lowered.

The magnetic material having the composition expressed by the formula(1) applies a mixture of element R1 and element R2 as the rare earthelement to lower the magnetic anisotropy. Therefore, a magnetic materialhaving a Curie temperature of 250K or more and 320K or less and showinga large magnetic entropy change amount (ΔS) at a relatively low magneticfield can be realized on the basis of the element R1 and the element R2.In order to obtain an increased effect of ΔS, the value y in the formula(1) is determined to fall in a range from 0.05 to 0.95. When the value yis not in this range, the mixing effect of the element R1 and theelement R2 cannot be obtained satisfactorily. It is preferable that thevalue y is in a range from 0.25 to 0.75 in order to obtain theimprovement effect of ΔS with better reproducibility.

The element R2 may be at least one selected from Ce, Pr, Nd, Tb and Dy.The use of at least one selected from Ce, Pr and Nd as the element R2enables to increase saturation magnetization of the magnetic material.The increase in saturation magnetization of the magnetic material formagnetic refrigeration contributes to the increase of ΔS. Therefore, theelement R2 preferably contains at least one selected from Ce, Pr and Ndin 70 atomic % or more of a total amount of the element R2. Besides, theelement R2 is more preferably at least one selected from Ce, Pr and Nd.

The magnetic material is not limited to the composition expressed by theformula (1) but may have a composition which has the element R or Fepartially replaced by another element. A part of the element R2 may bereplaced by at least one of element R3 selected from La, Gd, Ho, Y, Tmand Yb. The partial replacement of the element R2 by the element R3enables to control the magnetic anisotropy of the magnetic material andthe Curie temperature. But, if the replacement amount by the element R3is excessively large, the magnetic entropy change might be loweredconversely. Therefore, it is preferable that the replacement amount bythe element R3 is 20 atomic % or less of the element R2.

A part of Fe may be replaced by at least one of element M1 selected fromTi, V, Cr, Mn, Co, Ni, Cu, Zn, Zr, Nb, Mo, Hf, Ta, W, Al, Si, Ga and Ge.By partially replacing Fe by the element M1, the magnetic anisotropy canbe further lowered or the Curie temperature can be controlled. Theelement M1 is more preferably at least one selected from Ni, Co, Mn, Ti,Zr, Al and Si. But, if the replacement amount by the element M1 isexcessively large, magnetization is deteriorated, and the magneticentropy change is possibly lowered. Therefore, the replacement amount bythe element M1 is preferably 20 atomic % or less of Fe.

The magnetic material for magnetic refrigeration of the first embodimentincludes a composition having the rare earth element R in a smallamount, exhibiting a second order magnetic phase transition, having aCurie temperature near room temperature (e.g., 320K or less), andexhibiting a large magnetic entropy change (ΔS) at a relatively lowmagnetic field. Therefore, a magnetic material for magneticrefrigeration having high performance and excelling in practical utilitycan be provided at a low cost. Such a magnetic material for magneticrefrigeration is applied to a heat regenerator, a magnetic refrigerationdevice and the like. At that time, it can also be used in combinationwith, for example, the magnetic material exhibiting a first ordermagnetic phase transition.

The magnetic material for magnetic refrigeration according to a secondembodiment of the invention will be described. The magnetic material formagnetic refrigeration of the second embodiment has a compositionexpressed by the following general formula:

(R_(1-y)X_(y))_(x)Fe_(100-x)  (2)

(where, R is at least one of element selected from La, Ce, Pr, Nd, Sm,Gd, Tb, Dy, Ho, Er, Tm, Yb and Y, X is at least one of element selectedfrom Ti, Zr and Hf, and x and y are numerical values satisfying 4≦x≦20atomic 0 and 0.01≦y≦0.9), and includes a Th₂Ni₁₇ crystal phase or aTbCu₇ crystal phase as a main phase.

Similar to the first embodiment, the magnetic material for magneticrefrigeration of the second embodiment realizes a second order magneticphase transition by a material (material having the rare earth element Rin a small amount) which has rare earth element R and Fe as maincomponents and inexpensive Fe as a base. The R—Fe based magneticmaterial exhibits a second order magnetic phase transition with aninexpensive composition and has a Curie temperature near roomtemperature (e.g., Curie temperature of 250K or more and 320K or less)based on the selection of the element R. But, there is a possibilitythat a sufficient magnetic entropy change amount (ΔS) cannot be obtainedwhen only the R—Fe based composition is used.

The magnetic material for magnetic refrigeration of the secondembodiment has the rare earth element R partially replaced by an elementX (at least one of element selected from Ti, Zr and Hf) having an atomicradius smaller than that of the rare earth element R. Thus, by replacingthe rare earth element R partially by the element X, the Th₂Ni₁₇ crystalphase or the TbCu₇ crystal phase is stabilized. Accordingly,magnetization is increased, and a large magnetic entropy change amount(ΔS) can be obtained. In other words, the magnetic material of thesecond embodiment is inexpensive and excels in performance and practicalutility, and it is suitably used for the heat regenerator, the magneticrefrigeration device and the like. At that time, it can also be used incombination with the magnetic material exhibiting a first order magneticphase transition.

In order to obtain a replacement effect of the element X, the value y inthe formula (2) shall be in a range from 0.01 to 0.9. When the value yis less than 0.01, a stabilization effect of the Th₂Ni₁₇ crystal phaseor the TbCu₇ crystal phase by the replacement by the element X cannot beobtained sufficiently. When the value y exceeds 0.9, it is hard toproduce the Th₂Ni₁₇ crystal phase and the TbCu₇ crystal phase. The valuey is preferably in a range from 0.01 to 0.5. The value x shall be in arange from 4 to 20 atomic % in order to produce the Th₂Ni₁₇ crystalphase and the TbCu₇ crystal phase. When it deviates from the range, itis hard to produce the Th₂Ni₁₇ crystal phase and the TbCu₇ crystalphase. The value x is more preferably in a range from 8 to 15 atomic %.

The rare earth element R of the second embodiment may be at least oneselected from La, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho, Er, Tm, Yb and Y andnot limited to a special one. By using Ce, Pr, Nd, Sm or the like as therare earth element R, the saturation magnetization of the magneticmaterial can be increased. Therefore, the element R preferably containsat least one selected from Ce, Pr, Nd and Sm in 50 atomic % or more of atotal amount of the element R. Besides, the element R is more preferablycomposed of at least one selected from Ce, Pr, Nd and Sm.

The magnetic material of the second embodiment is not limited to thecomposition expressed by the formula (2) but may have a compositionwhich has Fe partially replaced by another element. A part of Fe may bereplaced by at least one of element M2 selected from V, Cr, Mn, Co, Ni,Cu, Zn, Nb, Mo, Ta, W, Al, Si, Ga and Ge. By replacing the Fe partiallyby the element M2, magnetic anisotropy, a Curie temperature and the likecan be controlled. The element M2 is more preferably at least oneselected from Ni, Co, Mn, Cr, V, Nb, Mo, Al, Si and Ga. But, if thereplacement amount by the element M2 is too large, magnetization isdecreased, and a magnetic entropy change might be decreased. Therefore,the replacement amount by the element M2 is preferably 20 atomic % orless of Fe.

The magnetic materials for magnetic refrigeration according to the firstand second embodiments are produced as follows. First, an alloycontaining prescribed amounts of individual elements is produced by anarc melting or an induction melting. For production of the alloy, arapid quenching method such as a single roll method, a double rollmethod, a rotary disk method or a gas atomization method, and a methodusing solid-phase reaction such as a mechanical alloying method may beapplied. The alloy can also be produced by a hot press, spark plasmasintering or the like of material metal powder without through a meltingprocess.

The alloy produced by the above-described method can be used as amagnetic refrigeration material depending on the composition, theproduction process and the like. Besides, the alloy is annealed, ifnecessary, so to control the constituent phase (e.g., single-phasing ofthe alloy), to control the crystalline particle diameter and to improvethe magnetic characteristic and then used as a magnetic refrigerationmaterial. An atmosphere in which melting, rapid quenching, mechanicalalloying and annealing are performed is preferably an inert atmosphereof Ar or the like in view of prevention of oxidation. The main phasecrystal structure can be controlled depending on a difference in theproduction method and production conditions. For example, in a casewhere a magnetic material is produced by the rapid quenching method orthe mechanical alloying method, the TbCu₇ crystal phase tends to beproduced.

Then, specific examples of the invention and evaluated results thereofwill be described.

EXAMPLES 1 TO 7

First, high-purity materials were blended at a prescribed ratio toprepare the compositions shown in Table 1, and mother alloy ingots wereproduced by an induction melting in an Ar atmosphere. The mother alloyingots were thermally treated in an Ar atmosphere at 1100° C. for tendays to produce magnetic materials for magnetic refrigeration. Theindividual magnetic materials were examined for appeared phases by X-raypowder diffraction to find that they had a Th₂Zn₁₇ crystal phase or aTh₂Ni₁₇ crystal phase as a main phase. The main phases of the individualmagnetic materials are shown in Table 1.

EXAMPLES 8 TO 11

Individual mother alloy ingots having the compositions shown in Table 1were produced in the same way as in Examples 1 to 7, and their motheralloys were partially used to produce quenched thin ribbons. Thequenched thin ribbons were produced by melting the alloys by inductionmelting in an Ar gas atmosphere and injecting the molten alloy onto arotating copper roll. The roll was determined to have a peripheralvelocity of 30 m/s. The obtained quenched thin ribbons (magneticmaterials for magnetic refrigeration) were examined for appeared phasesby X-ray powder diffraction to find that they had a Th₂Ni₁₇ crystalphase or a TbCu₇ crystal phase as a main phase. The main phases of theindividual magnetic materials are shown in Table 1.

COMPARATIVE EXAMPLES 1 TO 4

Single Gd (Comparative Example 1), an Sm₂Fe₁₇ based material(Comparative Example 2), a Ce₂Fe₁₇ based material (Comparative Example3), and an La(Fe, Si)₁₃ based material (Comparative Example 4) wereproduced in the same way as in Examples 1 to 7. The main phases of theindividual materials are shown in Table 1.

TABLE 1 Composition Main phase Example 1(Sm_(0.3)Er_(0.1)Pr_(0.5)Ce_(0.1))_(12.2)Fe_(87.8) Th₂Zn₁₇ Example 2(Sm_(0.3)Pr_(0.5)La_(0.2))_(11.5)Fe_(88.5) Th₂Zn₁₇ Example 3(Sm_(0.4)Er_(0.1)Nd_(0.5))_(12.0)(Fe_(0.9)Ni_(0.1))_(88.0) Th₂Zn₁₇Example 4 (Sm_(0.4)Er_(0.1)Dy_(0.5))_(8.0)(Fe_(0.9)Mn_(0.1))_(92.0)Th₂Ni₁₇ Example 5 (Sm_(0.3)Er_(0.1)Pr_(0.5)Gd_(0.1))_(15.0)Fe_(85.0)Th₂Zn₁₇ Example 6 (Er_(0.4)Ce_(0.2)Nd_(0.4))_(12.5)Fe_(87.5) Th₂Zn₁₇Example 7 (Sm_(0.5)Pr_(0.3)Tb_(0.2))_(12.0)Fe_(88.0) Th₂Zn₁₇ Example 8(Pr_(0.4)Sm_(0.5)Dy_(0.1))_(10.2)Fe_(89.8) TbCu₇ Example 9(Pr_(0.3)Sm_(0.5)Zr_(0.2))_(9.8)Fe_(90.2) Th₂Ni₁₇ Example 10(Pr_(0.3)Nd_(0.2)Zr_(0.4)Hf_(0.1))_(10.2) TbCu₇(Fe_(0.9)Ni_(0.05)Al_(0.05))_(89.8) Example 11(Ce_(0.2)Pr_(0.5)Zr_(0.2)Ti_(0.1))_(10.5)Fe_(89.5) TbCu₇ Comparative GdGd Example 1 Comparative Sm_(11.5)Fe_(88.5) Th₂Ni₁₇ Example 2Comparative Ce_(11.5)Fe_(88.5) Th₂Ni₁₇ Example 3 ComparativeLa_(6.7)(Fe_(0.88)Si_(0.12))_(86.6)H_(6.7) NaZn₁₃ Example 4

Then, the individual magnetic materials of Examples 1 to 11 andComparative Examples 1 to 4 were determined for a magnetic entropychange amount ΔS (T, ΔH) with an outer magnetic field varied frommagnetization measurement data by using the following formula. In theformula, T denotes a temperature, H denotes a magnetic field, and Mdenotes magnetization.

ΔS(T,ΔH)=∫(∂M(T,H)/∂T)_(H) dH(H;0→ΔH)

In any case, the ΔS indicates a peak for arbitrary ΔH at a prescribedtemperature (T_(peak)). The T_(peak) corresponds to a Curie temperature.Table 2 shows temperatures (T_(peak)) at which the magnetic entropychange amounts of the individual magnetic materials exhibit peaks,magnetic entropy change amounts (ΔS_(max) (absolute value)) for magneticfield changes (ΔH=1.0T) at T_(peak), and the temperature widths (ΔT)satisfying ΔS>ΔS_(max)/2 on the ΔS_(max)-T curve.

TABLE 2 T_(peak) |ΔS_(max)| ΔT (K) (J/kg · K) (K) Example 1 315 2.8 30Example 2 305 2.4 28 Example 3 300 2.6 23 Example 4 298 2.2 30 Example 5318 2.5 25 Example 6 290 2.4 28 Example 7 310 2.5 24 Example 8 Example 9295 2.7 26 Example 10 305 2.3 24 Example 11 310 2.5 29 ComparativeExample 1 295 3.2 28 Comparative Example 2 375 1.7 25 ComparativeExample 3 215 1.5 23 Comparative Example 4 277 16 7

It is apparent from Table 2 that the individual magnetic materials ofExamples 1 to 11 show ΔS_(max) and ΔT equivalent to those of Gd ofComparative Example 1 though a rare earth element is contained in asmall amount. It contributes greatly to provision of the magneticmaterial exhibiting a second order magnetic phase transition at a lowcost. Meanwhile, it is seen that Comparative Example 2 is poor inperformance because it has small ΔS_(max) though the ΔT shows a goodvalue. Comparative Example 3 is poor in T_(peak), ΔT and ΔS_(max). It isseen that the La(Fe, Si)₁₃ based material of Comparative Example 4 has arare earth element in a small amount and shows large ΔS_(max) but has asmall value ΔT and drawbacks in a practical view because it uses a firstorder magnetic phase transition.

Additional advantages and modifications will readily occur to thoseskilled in the art. Therefore, the invention in its broader aspects isnot limited to the specific details and representative embodiments shownand described herein. Accordingly, various modifications may be madewithout departing from the spirit or scope of the general inventiveconcept as defined by the appended claims and their equivalents.

1. A magnetic material for magnetic refrigeration, comprising: a composition represented by a general formula: (R1_(1-y)X_(y))_(x)Fe_(100-x) where, R is at least one of element selected from La, Ce, Pr, Nd, Sm, Gd, Tb, Dy, Ho, Er, Tm, Yb and Y, X is at least one of element selected from Ti, Zr and Hf, x is a value satisfying 4≦x≦20 atomic % and y is a value satisfying 0.01≦y≦0.9, wherein the magnetic material comprises a Th₂Ni₁₇ crystal phase or a TbCu₇ crystal phase as a main phase.
 2. The material according to claim 1, wherein the magnetic material exhibits a second order magnetic phase transition.
 3. The material according to claim 1, wherein the magnetic material has a Curie temperature of 320K or less.
 4. The material according to claim 1, wherein the element R comprises 50 atomic % or more of at least one selected from Ce, Pr, Nd and Sm.
 5. The material according to claim 1, wherein the element R comprises at least one selected from the group consisting of Ce, Pr, Nd and Sm.
 6. The material according to claim 1, wherein the value y is in a range from 0.01 to 0.5.
 7. The material according to claim 1, wherein a part of the Fe is replaced by at least one of element selected from the group consisting of V, Cr, Mn, Co, Ni, Cu, Zn, Nb, Mo, Ta, W, Al, Si, Ga and Ge.
 8. The material according to claim 1, wherein a part of the Fe is replaced by at least one of element selected from the group consisting of Ni, Co, Mn, Cr, V, Nb, Mo, Al, Si and Ga. 